determination of optimal reaction temperature and hydrogen...

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G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127 119 1 Introduction Polypropylene is nowadays one of the most widely used polyolefins, and its application is strongly influenced by the final product properties. In spite of about sixty years of Ziegler-Natta catalyst use for polypropylene production, the polymerization performance remains ambiguous and hazy due to the complexity of the catalyst kinetics. 1–2 In practice, the polymer application is determined by cer- tain crucial indices, such as the number and weight average molecular weight ( n M & w M ) and dispersity (Đ) as an indi- cator of molecular weight distribution. Since these indices of final product properties are highly dependent on the process variables, i.e., reaction temperature and hydro- gen amount in the polymerization system, it is necessary to investigate how the process variables affect these final product properties indices. Accordingly, for designing a desired product, a mathematical model could be a worthy replacement for the conventional manner, i.e., experimen- tal by trial and error. There is still a need for a validated mathematical model that would be able to predict these final product properties in a proper way. In view of the sig- nificance of these matters, few researchers have addressed these problems in a comprehensive and clarified manner, in particular with the aid of a validated mathematical mod- el. However, the gap remains. To understand the behaviour of the polymerization sys- tem, most studies so far have focused on the experimental approach. However, this approach is neither reliable nor applicable since its results are heavily dependent on the test and laboratory conditions. The other constraint of this approach is the type of catalyst used. 3–5 Therefore, these studies have not fulfilled the existing gap as defined earlier. In respect of the modelling, Reginato 2 modelled an in- dustrial-scale loop reactor using a non-ideal continuous stirred tank model to explain the industrial process, and compared their simulation results with commercial plant data. Al-haj Ali 3 proposed a generalized model for hydro- gen response based on the dormant site theory in liquid propylene polymerization. His research work was based on only experimental data, and there was no validated mathematical model able to predict the polymerization rate profile and the indices of the final product properties simultaneously. Although some other researchers in this field have carried out their work based on a mathematical model, there re- mains the defined gap, because their models have been es- tablished based on only mathematical calculations without experimental validation. In this context, some studies only tend to focus on loop or fluidized-bed reactors (FBRs), i.e., bulk or gas phase polymerization. 2,6–8 Yang 9 has modelled loop propylene polymerization reactors in bulk media. The model was targeted at commercial reactor variables with- out being attentive to kinetics studies and final product properties. Subsequently, another paper was published in- volving modelling of multi-scale polypropylene properties in the FBR reactor. Their modelling approach was moment equations. 10 Like in their in previous work, in 2016 Kim et al. 11 proposed a simulation for liquid polypropylene po- lymerization reactors based on Sheripol technology with- out giving attention to the determination of the vital final product properties, such as average molecular weight and polydispersity. Determination of Optimal Reaction Temperature and Hydrogen Amount for Propylene Polymerization by a Mathematical Model DOI: 10.15255/KUI.2018.038 KUI-9/2019 Original scientific paper Received August 1, 2018 Accepted December 17, 2018 G. H. Varshouee, a A. Heydarinasab, a* A. Vaziri, a and S. M. Ghafelebashi Zarand b This work is licensed under a Creative Commons Attribution 4.0 International License Department of Petroleum and Chemical Engineering, Science and Research Branch, Islamic Azad University, Tehran, Iran b Polymer Group, Research and Technology, National Petrochemical Company, Tehran, Iran Abstract Regarding the complexity of Ziegler-Natta catalyst kinetics in polypropylene polymerization, so far, there is no adequate mod- el to determine the best process conditions for predicting average molecular weight and dispersity as the most crucial final product properties index. Consequently, a validated model has been developed which describes the relationship between the kinetic model and the existing gap using the polymer moment balance approach. It was concluded that increasing reaction temperature and hydrogen amount are useful and improve the final product indices to a certain limit, but afterwards they have harmful effects on the indices. Keywords Mathematical modelling, propylene polymerization, optimization, population balance, average molecular weight, dispersity * Corresponding author: Assoc. Prof. Amir Heydarinasab Email: [email protected]

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Page 1: Determination of Optimal Reaction Temperature and Hydrogen ...silverstripe.fkit.hr/kui/assets/Uploads/IV-119-127.pdf · bulk or gas phase polymerization.2,6–8 Yang9 has modelled

G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127 119

1 IntroductionPolypropylene is nowadays one of the most widely used polyolefins, and its application is strongly influenced by the final product properties. In spite of about sixty years of Ziegler-Natta catalyst use for polypropylene production, the polymerization performance remains ambiguous and hazy due to the complexity of the catalyst kinetics.1–2

In practice, the polymer application is determined by cer-tain crucial indices, such as the number and weight average molecular weight ( nM & wM ) and dispersity (Đ) as an indi-cator of molecular weight distribution. Since these indices of final product properties are highly dependent on the process variables, i.e., reaction temperature and hydro-gen amount in the polymerization system, it is necessary to investigate how the process variables affect these final product properties indices. Accordingly, for designing a desired product, a mathematical model could be a worthy replacement for the conventional manner, i.e., experimen-tal by trial and error. There is still a need for a validated mathematical model that would be able to predict these final product properties in a proper way. In view of the sig-nificance of these matters, few researchers have addressed these problems in a comprehensive and clarified manner, in particular with the aid of a validated mathematical mod-el. However, the gap remains.

To understand the behaviour of the polymerization sys-tem, most studies so far have focused on the experimental approach. However, this approach is neither reliable nor applicable since its results are heavily dependent on the

test and laboratory conditions. The other constraint of this approach is the type of catalyst used.3–5 Therefore, these studies have not fulfilled the existing gap as defined earlier.

In respect of the modelling, Reginato2 modelled an in-dustrial-scale loop reactor using a non-ideal continuous stirred tank model to explain the industrial process, and compared their simulation results with commercial plant data. Al-haj Ali3 proposed a generalized model for hydro-gen response based on the dormant site theory in liquid propylene polymerization. His research work was based on only experimental data, and there was no validated mathematical model able to predict the polymerization rate profile and the indices of the final product properties simultaneously.

Although some other researchers in this field have carried out their work based on a mathematical model, there re-mains the defined gap, because their models have been es-tablished based on only mathematical calculations without experimental validation. In this context, some studies only tend to focus on loop or fluidized-bed reactors (FBRs), i.e., bulk or gas phase polymerization.2,6–8 Yang9 has modelled loop propylene polymerization reactors in bulk media. The model was targeted at commercial reactor variables with-out being attentive to kinetics studies and final product properties. Subsequently, another paper was published in-volving modelling of multi-scale polypropylene properties in the FBR reactor. Their modelling approach was moment equations.10 Like in their in previous work, in 2016 Kim et al.11 proposed a simulation for liquid polypropylene po-lymerization reactors based on Sheripol technology with-out giving attention to the determination of the vital final product properties, such as average molecular weight and polydispersity.

Determination of Optimal Reaction Temperature and Hydrogen Amount for Propylene Polymerization by a Mathematical Model

DOI: 10.15255/KUI.2018.038 KUI-9/2019

Original scientific paperReceived August 1, 2018

Accepted December 17, 2018

G. H. Varshouee,a A. Heydarinasab,a* A. Vaziri,a and S. M. Ghafelebashi Zarand b

This work is licensed under a Creative Commons Attribution 4.0

International License

a Department of Petroleum and Chemical Engineering, Science and Research Branch, Islamic Azad University, Tehran, Iranb Polymer Group, Research and Technology, National Petrochemical Company, Tehran, Iran

AbstractRegarding the complexity of Ziegler-Natta catalyst kinetics in polypropylene polymerization, so far, there is no adequate mod-el to determine the best process conditions for predicting average molecular weight and dispersity as the most crucial final product properties index. Consequently, a validated model has been developed which describes the relationship between the kinetic model and the existing gap using the polymer moment balance approach. It was concluded that increasing reaction temperature and hydrogen amount are useful and improve the final product indices to a certain limit, but afterwards they have harmful effects on the indices.

KeywordsMathematical modelling, propylene polymerization, optimization, population balance, average molecular weight, dispersity

* Corresponding author: Assoc. Prof. Amir HeydarinasabEmail: [email protected]

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G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127120

In 2018, Varshouee et al. focused on providing a validated model that would be able to predict and plot the polymeri-zation profile.12 Their aim was to evaluate the performance of the used catalyst with changing process variables, such as reaction temperature and hydrogen amount in the sys-tem, in view point of the kinetic study. Since the profile rate of the polymerization is necessary for determination of the yield (Y) and deactivation constant (KD) of the cat-alyst, they explain these matters by a validated model.13 They concluded that, according to the Arrhenius theory, an increase in temperature leads to an increase in the po-lymerization rate.12 Regarding the effect of hydrogen on the kinetics, their model showed that increasing hydrogen amount not only increases the rate of polymerization, but also significantly raises the percentage of the activated site on the catalyst. For instance, in the absence of hydro-gen, only 10.4 % of the potential active sites are activated for the reaction, while at 18 mg hydrogen content in the system, the percentage of the activated sites of the used catalyst reaches 85.5 %. However, the increasing reaction temperature and hydrogen amount have an optimum ef-fect, which should be determined carefully, because above the optimum condition, they have a harmful effect on the catalyst.12–13 Consequently, they decided to expand their model to cover the existing gap mentioned previously.

Having that in mind, we attempted to propose a vali-dated model that fulfils these aims, i.e., evaluate the ef-fect of reaction temperature and hydrogen amount on the number and weight average molecular weight ( nM& wM ) and dispersity (Đ) from the product properties viewpoint. By using the results of this study, the catalyst makers will be able to evaluate and improve their catalyst. It also might be attractive and essential for process engi-neers aiming at replacing new catalyst, increasing plant efficiency, improving product quality, reducing operating costs, and generating new formulation for economical products. Therefore, this study could be applied in basic and applied research. The selected modelling approach is polymer moment balance method (population balance approach) in MATLAB® & Simulink® software program for slurry polymerization. The model was validated through the experimental data from a lab-scale semi-batch reactor using the 4th generation of Ziegler-Natta catalysts with an acceptable margin of error.

2 Experimental 2.1 Material specifications

The materials used in this study were as follows. The cat-alyst used was the 4th generation of spherical MgCl2 sup-ported Ziegler-Natta catalyst containing 3.6 wt% of Ti; diisobutyl phthalate (DIBP) as internal donor supplied by Sudchemie, Germany. Triethylaluminium (TEAL of 98 % purity) from Merck, Germany, diluted in n-heptane was used as a co-catalyst. Cyclohexyl methyl dimethoxy silane (CMDS) purchased from Merck, Germany, was used as an external donor. Polymer-grade propylene was provided from Shazand Petrochemical, Iran. Hydrogen and nitrogen used were of >99.999 % purity.12–13

2.2 Experimental polymerization procedure

In this study, slurry homo-polymerization was carried out in heptane media. Polymerization reactor was a one-litre stainless steel vessel manufactured by Buchi. Polymeriza-tion set-up was designed in order to conduct slurry polym-erization in one vessel. A schematic diagram of polymer-ization set-up is shown in Fig. 1. A high-pressure N2 line was used to transfer liquid monomer and catalytic system into the reactor.

catalyst

computer

PID Controller

MFCPI

TI

vacuumnitrogen

purgehydrogen

injection

jacket out

propylene

jacket in

Fig. 1 – Simplified schematic of the reactor system

The catalyst system was injected into the reactor through a stainless steel cylinder under N2 atmosphere. All gases were first purified online by passing through three puri-fication trains (containing molecular sieves) in series. The individual gases were then filtered, and flow of each re-actant was measured and controlled with a Mass Flow Controller manufactured by Brooks. Experimental profile polymerization (Rp) curves come from set-up monitor, the molecular weight of products was measured by gel perme-ation chromatography (GPC) employing an Agilent PL-220 model with TSK columns at 155 °C using 1,2,4-trichloro-benzene as a solvent. The GPC was calibrated with the narrow molecular weight distribution polystyrene standard as a reference.

A typical polymerization procedure exists for reactor preparation, polymerization, and discharge. The detailed procedure of the polymerization was according to ref.13

2.2 Mathematical modelling

2.2.1 Assumptions

The following modelling assumptions were considered: (1) Propylene polymerization is carried out in the amorphous phase, and amorphous phase concentration during poly-propylene polymerization is at thermodynamic equilibri-um condition that obeys that from Sanchez and Lacombe

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G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127 121

equation (SLE) for calculating the amount of the hydrogen molar ratio (x = CH/Cm).14 (2) γ1 = γ2 =.....= γNC, where γ is equilibrium constant, and NC is the number of solvent in slurry phase components.2 (3) The reaction tempera-ture, pressure, and monomer concentration is kept con-stant during the polymerization process. (4) The resistance of mass and heat transfer, and the diffusion effect of the reactants is ignored. (5) The propagation constant is inde-pendent of the length of the growing polymer chain.

2.2.2 Mathematical formulas and equations

In respect to olefin polymerization, kinetics with Ziegler-Natta catalysts might be fairly complicated.2 To date, several reaction steps have been proposed in the open literature.2,6 The ODE mass balance equations2 used in this model were as follows (Eq. 1):

where for j = 1,2,....,NC

for j = 1,2,....,NC

(1)

, where:

Qf, Q0, and QR are feed volumetric flow rate, reactor-out-put volumetric flow rate, and volumetric recirculation flow rate, respectively. In Eq. 1, VR and Rj are defined as a reac-tor volume, and j as component reaction rate.

Since the model is a semi-batch process and constant mon-omer concentration during the polymerization is assumed, the input and output terms are eliminated (Qf and Q0), and therefore the terms η and ζ are meaningless for our study. Table 1 shows possible reactions with their rate equations in the polymerization reactor. The concentration variations with time used in modelling were as follows:

where k is the site number of the catalyst.

In this study, it was assumed that the catalyst has mono-site, and therefore, k is equal to one. Here, CH, CA, CE, CMi, CB, CS, Ccat, and P0 are the concentrations of hydrogen, co-cat-alyst (aluminum alkyl), electron donor, monomer, poison, site transfer, catalyst, and potential site in the polymeriza-tion, respectively. The component rate equations and mo-ment equations used in the model are listed in Table 2. The final product properties of polypropylene can be estimated by the moment equations. Evaluating the vital final prod-uct properties in this study, i.e., number average molecular weight ( nM ) and weight average molecular weight ( wM ) could be calculated by the following equations:

Table 1 – Probable reactions and their rate equations in propylene polymerization used in the model2

Reaction step Component Reaction Rate equation

site activation hydrogen (1)

Al-alkyl (2) = ,KaAOK k

aA aA p A aR k C C

monomer i (3) + → +0K

p i iC M P M =KaMiOK k

aMi aMi p MiR k C C

chain initiation monomer i (4) =0 0 0 ,i

K k KP i P i M aR k P C

chain propagation monomer j (5) = , ,j

K k KPji Pji n j M aR k P C

chain transfer hydrogen (6) + → +, 2 0

KhK K k

n i nP H P D =,, ,

KcHiOK n k K

cHi cHi n i H aR k P C

monomer j (7) = ,,, ,

KcMj i

ji ji

OK n k KcM cM n i j aR k P C

site deactivation hydrogen (8) + → +, 2K k

n i d nP H C D =,, ,

KdHOK n k K

aHi dH n i H aR k P C

+ →0 2K

dP H C =0 0 ,KdHOK k K

dH dH H aR k P C

Al-alkyl (9) + → +,K k

n i d nP A C D =,, ,

KdAOK n k K

dAi dA n i A aR k P C

spontaneous (10) → +,K k

n i d nP C D =,,

K n k KdSpi dSp n iR k P

→0K

dP C =0 0K k KdSp dSpR k P

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G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127122

(2)

(3)

then: (4)

2.2.3 Modelling algorithm

In this study, we outlined the algorithm for programming the mathematical model in a MATLAB® & Simulink® envi-ronment, as shown in Fig. 2A. It is composed of two parts; main-program (named “Runsim”) and subroutine (function file). For obtaining kinetic constants in the model, we pro-pose a new approach as iterative method algorithm using consistency property of ODE’s equation in Fig. 2B. The ad-vantage of this method is that it is easier and more reliable than conventional methods, i.e., referring directly to open literature or estimating by trial and error.2

Table 2 – Component rate and moment equations used in the model2

Hydrogen

Co-catalyst

Electron donor

Poison

Potential sites

Dead sites

Monomer

Moments equations:

Live polymer

Dead polymer where

Live moment

Bulk moment

Zero-order; live polymer moments

First-order; live polymer moments

Zero-order; bulk polymer moments

First-order; bulk polymer moment

Second-order; bulk polymer moment

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G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127 123

To use the iterative method algorithm, only the initial guess of kinetic constants should be estimated by referring to the open literature. Afterwards, the kinetic constants are ad-justed for the catalyst used by the algorithm.

In this study, the initial guess of kinetic constants was estimated and applied to the model from open litera-ture.2,6 Then, the constants were exactly adjusted and determined in accordance with the catalyst used in the set-up (experimental data) by the proposed algorithm in Fig. 2B.

3 Results and discussionAs outlined in the introduction, in order to cover the defined targets, i.e., evaluate the effect of reaction tem-perature, hydrogen amounts on the number and weight average molecular weight ( wM and nM ), and dispersity (Đ) from the viewpoint of the product properties, it was necessary to develop our previous work to be suitable in this regard.

The model was coded in MATLAB® & Simulink® software program, according to the algorithm shown in Fig. 2A. The reaction equation used in the model is listed in Table 1, and the components rate and moment equation used in the model are summarized in Table 2.

One of the most important advantages of this model is that it is able to show the profile rate of the polymerization graphically, and therefore, it is possible to compare the model profile and the experimental profile rates coming from the lab set-up. By having the profile rate of the po-lymerization, it is easily possible to study the kinetics of

Table 3 – Comparison of the model output and experimental results under different conditions

Recipe Results (experimental/model)Run No. T ⁄ °C H2 ⁄ mg Molar ratio

x = CH2/CmCatalyst ⁄ mg Y ⁄ g PP Mn Mw Đ

1 65 0 0 20Experimental result 63.29 210259 863057 4.1Model result 65.13 205570 834523 4.06Error ( % ) 3 2 3 1

2 70 0 0 20Experimental result 72.66 304642 1134374 3.71Model result 76.4 323780 1214440 3.75Error ( % ) 5 6 7 1

3 75 0 0 20Experimental result 63.07 236154 1124367 4.76Model result 67.25 270243 1178300 4.36Error ( % ) 6 13 5 9

4 70 18 0.00466 10Experimental result 81.33 29962 144192 4.81Model result 88.4 32812.7 148874 4.54Error ( % ) 8 9 3 6

5 70 27 0.00703 10Experimental result 74.61 24016 116939 4.87Model result 76.81 24981.1 123303 4.94Error ( % ) 3 4 5 1

x – hydrogen molar ratio is calculated by Aspen Software polymer software based on SLE (SOE)

start a)

b)

Input data (recipe condition): volume of solvent (l), temperature of reactor,

catayst (mg), co-catalyst (mg), H2 (mg), time (s), and reactor volume

selected EOS: Sanchez-Lacobe equation (SLE)to calculate molar ratios, reactor pressure (PR)

monomer and polymer properties

initial conditions

ODE's solution

shown outputs: Mn, Mw, Đare plotted curves

the rate constants of reactionsfrom handbooks/open literature

objectives final product properties such as Mn, Mw, Đ, etc.

experimental result from set-up/pilot plant

simulation programMATLAB® & Simulink®

Model calculated:1. profile rate curve of the polymerization2. final product propertiesW.Mw, N.Mw, Đ

Experimental data:1. profile rate curve of the po-

lymerization (from setup)2. final properties (from GPC)

W.Mw, N.Mw3. Đ = W.Mw ⁄ N.Mw

subroutine(function file)

Mai

n-pr

ogra

m(n

amed

“Ru

nsim

”)Co

nt. M

ain-

prog

ram

(nam

ed “

Runs

im”)

shown outputs:W.Mw, N.Mw, Đ

compared;are the errorsacceptable?

do you want more

information?

is error tolerance

OK?

finished

finished

finished

modified

No

No

Yes

ODE's

open literature as initial guess

kinetic constants

use iterative methodology

Fig. 2b

Fig. 1 – (a) General algorithm modelling in this work; (b) Itera-tive methodology used for adjusting kinetic parameters

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G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127124

the polymerization and determine the crucial indices that belong to the kinetics study.12–13

The experimental condition runs are listed under the title “recipe conditions”. In addition, the results from the model and experimental are summarized in detail in Table 3.

As shown in Figs. 3A–3B and 4A–4B, the comparison of the polymerization profile rate of the model outputs and the experimental data implies that fairly accurate kinetic constants have been adjusted and applied in the model, meaning that the performance of the designed algorithms for this study, i.e., Figs. 2A–2B are fairly suitable in this study.

From Figs. 3A–3B and 4A–4B, it can easily be concluded that the model performance is acceptable and the existing errors could be justified as follows:

(1) The global error that is the summation of truncation, method, and round off error.

(2) Personal and measurement equipment errors.(3) The equation of state was selected. (4) The assumption errors.

As may be seen from Fig. 3A, an increase in temperature increased the rate of polymerization in the absence of hydrogen, while under this condition only 10.4 % of the potential sites on the catalyst were activated.12 This phe-nomenon can easily be explained by Arrhenius theory. In the absence of hydrogen, the best reaction temperature is 70 °C because maximum yield and minimum deactiva-tion constant (KD) of the used catalyst have been observed

and the model could predict this event properly.13 Fig. 5A shows which changes in average molecular weight with temperature follow from a parabolic curve along with a maximum point at 70 °C. Fig. 3A shows the comparison of the experimental and model profile rates in the absence of hydrogen at different temperatures, i.e., the optimum temperature condition. In contrast, Fig. 5B shows the vari-ations of dispersity (Đ) as an indicator of molecular weight distribution, which also has a parabolic curve along with a minimum point at 70 °C. Lower Đ means that molecular weight distribution tends to narrow distribution. This can be justified due to the fact that catalyst has a maximum yield at 70 °C, see Table 3.

Hydrogen, as chain transfer agent, affects the kinetics of propylene polymerization. Consequently, variations in hy-drogen concentration lead to the change in final product properties and activated sites of used catalyst.

Fig. 4B displays the polymerization profile rates at the dif-ferent hydrogen concentration and in the polymerization system. It shows that increased hydrogen concentration raises the peak, i.e., the presence of hydrogen causes more activated sites of the catalyst to a specific limit. This issue can be justified by dormant site theory.12 Above the spe-cific limit, the activated sites of the catalyst are gradually reduced because of the excess hydrogen amounts above the specified limit, as chain transfer agent is able to react with activated sites of the catalyst. Therefore, it is expected that activated sites of the catalyst will be reduced.

These arguments are confirmed by referring and precise-ly evaluating Figs. 6A–6B, regarding the changes in aver-

t ⁄ h

0

1

2

3

4

5

6

7

8 Quasy Steady State zoneInitialzone

75 °C

70 °C65 °C

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2

R p ⁄

kg g(

cat)−

1 h−

1

model

(A)

experimental

t ⁄ h

0

1

2

3

4

5

6

0 0.5 1 1.5 2

R p ⁄

kg g(

cat)−

1 h−

1

modelexperimental

Quasy Steady State zoneRun 2; 70 °C/NO H2 (B)

Initialzone

Fig. 3 – Comparison of the experimental and model profile rates in the absence of hydrogen at different temperatures; (A) Runs 1, 2, and 3; (B) Run 2 (optimum temperature)

t ⁄ h0123456789

10

0 0.5 1 1.5 2

R p ⁄

kg g(

cat)−

1 h−

1

modelexperimental

18 mg H2 (B)

t ⁄ h

0

2

4

6

8

10

12

0 0.5 1 1.5 2

R p ⁄

kg g(

cat)−

1 h−

1

modelexperimental

27 mg H2

18 mg H2

0 mg H2

(A)

Fig. 4 – Comparison of the experimental and model profile rates at 70 °C and different hydrogen amounts; (A) Runs 2, 4, and 5, (B) Run 4 (optimum condition)

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G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127 125

age molecular weight and dispersity (Đ) with hydrogen amount. It was concluded that in Fig. 6A, from point A to B, the hydrogen role is a chain transfer agent for activating sites on the catalyst. Consequently, the average molecu-lar weight is increased and due to the rapid increase in activated sites by rising hydrogen amount, the number of chains is also increased. Therefore, dispersity (Đ) has in-creases according to Fig. 6A. In Fig. 6A after point B, excess hydrogen amount reacts with the active site on the catalyst. As expected, the condition would be reversed, which is clearly shown in Figs. 6A–6B, thus point B or 70 °C and 18 mg hydrogen content (Run 4) could be considered as the optimum condition. Fig. 4A shows the comparison of the experimental and model profile rates in the presence of hydrogen (18 mg) at the optimum temperatures (70 °C). Consequently, Run 4 could be considered the optimum condition in this study.

The significant conclusions in this regard could be listed as follows:

1. If hydrogen concentration is below the optimum con-dition, by changing the hydrogen concentration, the process engineer could produce a wide range of aver-age molecular weight of the polymer based on the tai-lor-made product (see Fig. 6A point A to B).

2. At the optimum hydrogen concentration for the poly-propylene yield, the minimum average molecular weight is produced.

3. At the above optimum hydrogen concentration, excess hydrogen reacts with the activated site on the used cata-

lyst. Therefore, the consumption of the catalyst increas-es, which is an undesirable event.

4. Existing hydrogen in system generally reduces the av-erage molecular weight. The significance of this issue depends on the process engineer targets.

It is worth emphasizing that the behaviour of each Ziegler-Natta catalyst depends on the user’s process con-ditions and recipe. The novelty in this study is that the proposed model could be able to determine the optimum process conditions based on tailor-made products, replace new catalyst and accessible catalyst with acceptable accu-racy.

4 ConclusionThe present work aimed to provide a validated mathemat-ical model to predict and evaluate the effect of reaction temperature and hydrogen amount on the number and weight average molecular weight ( wM & nM ) and disper-sity (Đ) from the viewpoint of the product properties. For this purpose, two algorithms were outlined – the first algo-rithm, i.e., Fig. 2A was used for the main program; and the second algorithm, i.e., Fig. 3A was applied for tuning and adjusting the constants of kinetic equations based on the Ziegler-Natta catalysts. By using the results of this study, the catalyst makers will be able to evaluate and improve their catalyst. In addition, this study might be attractive and es-sential for process engineers aiming at replacing new cata-

64 66 68 70 72 74 76T ⁄ °C

Đ

3.003.203.403.603.804.004.204.604.604.805.00

model

In absence of hydrogen

experimental

64 66 68 70 72 74 76T ⁄ °C

Mw ⁄

kg gm

ol−

1

Mn ⁄

kg gm

ol−

1

0

200000

400000

600000

800000

1000000

1200000

1400000

0

200000

400000

600000

800000

1000000

1200000model

model

experimental

experimental

Mn

Mw

(B)

(A)

Fig. 5 – (A) Comparison of the experimental and model out-put Mn and Mw, in the absence of hydrogen at different temperatures; (B) comparison of the experimental and model outputs of Đ in the absence of hydrogen at dif-ferent temperatures

0 5 10 15 20 25 300

200000

400000

600000

800000

1000000

1200000

0

100000

200000

300000

400000

5000000

7200000

6200000

Mw ⁄

kg gm

ol−

1

Mn ⁄

kg gm

ol−

1

hydrogen mass ⁄ mg

experimental

Mn

Mw

A

B

model

model

(A)

0 5 10 15 20 25 30hydrogen mass ⁄ mg

(B)

Đ

3.00

3.50

4.00

4.50

5.00

5.50

experimental

model

Fig. 6 – (A) Comparison of the experimental and model outputs regarding Mw and Mn, with changing hydrogen amount at 70 °C; (B) comparison of the experimental and model outputs of Đ in the presence of different hydrogen con-centrations at constant temperature of 70 °C

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G. H. VARSHOUEE et al.: Determination of Optimal Reaction Temperature and Hydrogen ..., Kem. Ind. 68 (3-4) (2019) 119–127126

lyst, increasing plant efficiency, improving product quality, reducing operating costs, and generating new formulation for economical products. Therefore, this study could be applied in basic and applied research. The software pro-gram was coded in MATLAB® & Simulink® and validated by the experimental data from a lab setup reactor.

The comparison of the model outputs and experimental results shows that both results are in accordance with each other in an acceptable margin of error. Finally, it was con-cluded that the optimum condition in this study was 70 °C and 18 mg of hydrogen content.

The main aim of this study was to gain a considerable in-sight into the Ziegler-Natta catalyst performance by chang-ing variables.

List of abbreviations and symbols

C – total active site concentration, mol dm−3

Cd – dead-site concentration, mol dm−3

Cj – component j bulk concentration, mol dm−3

Cj,R – concentration into the reactor, mol dm−3

Ck – type k active specie concentration, mol dm−3

Cp – potential site concentration, mol dm−3

Dkn – dead polymer chain concentration with n monomers originated from site k, mol dm−3

Đ – dispersityK – two-site equilibrium constant, kg mol−1

Mw – mass average molecular weight, kg mol−1

NC – number of liquid-phase componentsnj,R – moles of component j into reactornj,a – moles of j sorbed in the amorphous polymer phasenj,l – moles of j in the liquid phaseNm – number of monomersNs – number of sitesOrk – order of reaction r for site kPn,ik – growing polymer chain with n monomers

with end-group i from site k, mol dm−3

P0k – vacant site k concentration, mol dm−3

Rp – polymerization rate, kg g(cat)−1 h−1

Rp0 – initial polymerization rate, kg g(cat)−1 h−1

t – time, sTr – reactor temperature, KTf – feed stream temperature, KVR – reactor volume, m3

Y – yield, g PPRrk,n – r reaction from site k for a growing chain with n

monomers, mol m−3 s−1

Rj – j component reaction rate, mol m−3 s−1

γj – equilibrium constant for j component between liquid phase and amorphous polymer phase

ξ – ratio between solid-phase components concentration at reactor output flow and into reactor

η – ratio between liquid-phase components concentration at reactor output flow and into reactor

χ – volume fraction of monomer in the amorphous polymer phase

ρl – liquid-phase density, kg m−3

ρp – polymer density, kg m−3

ρR – reactor slurry density, kg m−3

– live moment rate equations

– bulk moment rate equations

References

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8. J. J. C. Samson, P. J. Bosman, G. Weickert, K. R. Westerterp, Liquid‐phase polymerization of propylene with a highly ac-tive Ziegler–Natta catalyst. Influence of hydrogen, cocatalyst, and electron donor on the reaction kinetics, J. Polym. Sci. Part A 37 (1999) 219, doi: https://doi.org/10.1002/(SICI)1099-0518(19990115)37:2<219::AID-POLA12>3.0.CO;2-3.

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SAŽETAKOdređivanje optimalne temperature reakcije i udjela vodika

za polimerizaciju propilena matematičkim modelomGholam Hossain Varshouee,a Amir Heydarinasab,a* Ali Vaziri,a

and Seyed Mehdi Ghafelebashi Zarand b

S obzirom na kinetičku složenost Ziegler-Natta katalizatora u polipropilenskoj polimerizaciji, za sada ne postoji odgovarajući model za određivanje optimalnih uvjeta procesa za predviđanje prosječne molekularne mase i disperzije kao najvažnijih indeksa svojstava konačnog proizvoda. Slijedom toga, razvijen je validirani model koji opisuje odnos između kinetičkog modela i posto-jećeg jaza pristupom ravnoteže momenata. Zaključeno je da su povišena temperatura reakcije i količina vodika korisni i do određene granice poboljšavaju indekse gotovog proizvoda, ali nakon toga na indekse imaju štetni učinak.

Ključne riječi Matematičko modeliranje, polimerizacija propilena, optimizacija, populacijska ravnoteža, prosječna molekularna težina, disperznost

Izvorni znanstveni radPrispjelo 1. kolovoza 2018.

Prihvaćeno 12. prosinca 2018.

a Department of Petroleum and Chemical Engineering, Science and Research Branch, Islamic Azad University, Tehran, Iran

b Polymer Group, Research and Technology, National Petrochemical Company, Tehran, Iran